金属材料辐照缺陷演化的分子动力学研究进展

辐照条件下,高能粒子在金属材料内部引入稠密的辐照缺陷,导致材料力学性能严重退化,缩短材料服役寿命,是辐照材料研究的关键问题。辐照缺陷多处在纳米尺度,故分子动力学方法是模拟辐照缺陷的有力工具,近年来被广泛用于研究辐照缺陷演化。本文总结了金属材料中辐照缺陷演化的分子动力学研究进展,介绍了级联碰撞、点缺陷、空洞、氦泡、Frank位错环、层错四面体等辐照缺陷,及其与位错、晶界等微结构的相互作用。分子动力学方法揭示的机制与模型,深化了学界对辐照效应的认识,有助于提高辐照材料力学性能和设计耐辐照材料。     

金属材料辐照缺陷演化的分子动力学研究进展

辐照条件下,高能粒子在金属材料内部引入稠密的辐照缺陷,导致材料力学性能严重退化,缩短材料服役寿命,是辐照材料研究的关键问题。辐照缺陷多处在纳米尺度,故分子动力学方法是模拟辐照缺陷的有力工具,近年来被广泛用于研究辐照缺陷演化。本文总结了金属材料中辐照缺陷演化的分子动力学研究进展,介绍了级联碰撞、点缺陷、空洞、氦泡、Frank位错环、层错四面体等辐照缺陷,及其与位错、晶界等微结构的相互作用。分子动力学方法揭示的机制与模型,深化了学界对辐照效应的认识,有助于提高辐照材料力学性能和设计耐辐照材料。     

激光辐照诱导的热与力学效应

对激光辐照诱导的热与力学问题研究进展进行了综述,包括材料在高温、高升温速率下的本构关系,典型薄板和柱壳等结构在激光辐照下的热力破坏效应,多层材料体系的激光破坏行为等几个方面,并着重介绍了包含相变与烧蚀过程的激光破坏分析模型与机制研究,激光辐照效应的流–热–固耦合数值模拟方法,以及短脉冲激光引起的冲击与破坏机理等方面的研究新进展。     

Progress in thermal-mechantical effects induced by laser

对激光辐照诱导的热与力学问题研究进展进行了综述,包括材料在高温、高升温速率下的本构关系,典型薄板和柱壳等结构在激光辐照下的热力破坏效应,多层材料体系的激光破坏行为等几个方面,并着重介绍了包含相变与烧蚀过程的激光破坏分析模型与机制研究,激光辐照效应的流-热-固耦合数值模拟方法,以及短脉冲激光引起的冲击与破坏机理等方面的研究新进展.     

激光辐照诱导的热与力学效应

对激光辐照诱导的热与力学问题研究进展进行了综述,包括材料在高温、高升温速率下的本构关系,典型薄板和柱壳等结构在激光辐照下的热力破坏效应,多层材料体系的激光破坏行为等几个方面,并着重介绍了包含相变与烧蚀过程的激光破坏分析模型与机制研究,激光辐照效应的流–热–固耦合数值模拟方法,以及短脉冲激光引起的冲击与破坏机理等方面的研究新进展.     

充内压圆柱壳在激光辐照下的初始裂纹萌生机制研究

通过高速摄影在实验中观测到充压柱壳上初始裂纹萌生于激光辐照区中心．通过数值模拟、断口分析和激光辐照区材料的金相分析等手段揭示了裂纹初始萌生的物理力学机制，并进一步证实了裂纹初始萌生位置的问题．根据研究结果，确定了影响裂纹起始萌生的力学量．本项目工作的完成有助于激光辐照下充压柱壳断裂问题的深入研究．     

基于详细化学反应动力学的激光点火模型

为研究含能材料在激光作用下的点火特性,从基本守恒方程组出发,基于详细化学反应动力学模型,建立了含能材料激光点火的气相模型.利用所建立的模型对RDX在激光辐照下的点火过程进行了数值模拟,得到了点火过程中的瞬时温度分布和组分分布,对点火特性进行了分析.计算得到的不同激光功率密度下的RDX点火延迟时间与文献结果一致.     

飞秒激光对金属材料表面烧蚀区的XRD分析

在激光脉冲宽度为30fs,重复频率为10Hz,靶面处激光功率密度为1013W/cm2条件下,开展了真空中飞秒激光对铝、铜材料的烧蚀效应研究。对材料表面烧蚀区进行X射线衍射分析的结果表明,材料的表面烧蚀区没有发生相变,X射线的反射强度发生变化,但该区晶面对X射线的反射强度随激光功率密度的增加发生了变化,其衍射峰处出现了明显的展宽并出现分叉,说明该区域的不同晶面对飞秒激光的吸收具有明显的取向作用。     

飞秒激光辐射纳米薄膜脱附的能量输运机理研究

从微观能量传输角度,对飞秒脉冲激光的辐射传热及其产生的金属薄膜吸附层分子脱附过程的能量输运机理进行了研究。以非平衡态传热和随机过程理论为基础,建立了描述吸附分子脱附过程的数学模型;并分别对单脉冲与双脉冲飞秒激光辐射下,金属Ru基体表面层的电子和声子的温度分布、吸附层分子CO的脱附概率分布进行了数值模拟。其结果与实验规律相符,为飞秒脉冲激光应用于微机电系统中杂质脱附提供了重要信息。     

脉冲X射线辐照材料引起的汽化反冲冲量

分析比较了计算Ｘ射线辐照固体材料引起汽化反冲冲量的几种计算公式。通过对Ｘ射线辐照后材料运动过程的数值模拟和分析，提出了一种计算汽化反冲冲量的数值计算公式。计算结果表明:数值计算得到的汽化反冲冲量与ＢＢＡＹ公式的结果比较接近；脉冲Ｘ射线引起的汽化反冲冲量与Ｘ射线的能谱及辐照量有明显的依赖关系，且汽化反冲冲量随辐照量的变化是非线性的。     

The 7th International Conference on Fluid Mechanics May 24-27,2015,Qingdao,China

正http://www.icfm7.org First Announcement and Call for PapersThe objective of International Conference on Fluid Mechanics(ICFM)is to provide a forum for researchers to exchange new ideas and recent advances in the fields of theoretical,experimental,computational Fluid Mechanics as well as interdisciplinary subjects.It was successfully convened by the Chinese Society of Theoretical and Applied Mechanics(CSTAM)in Beijing(1987,     

INFORMATION FOR CONTRIBUTORS

Contributions： The Journal, Acta Mechanica Solida Sinica, is pleased to receive papers from engineers and scientists working in various aspects of solid mechanics. All contributions are subject to critical review prior to acceptance and publication.     

Preface

This special issue of PARTICUOLOGY is devoted to the first UK-China Particle Technology Forum taking place in Leeds, UK, on 1-3 April 2007. The forum was initiated by a number of UK and Chinese leading academics and organised by the University of Leeds in collaboration with Chinese Society of Particuology, Particle Technology Subject Group （PTSG） of the Institution of Chemical Engineers （IChemE）, Particle Characterisation Interest Group （PCIG） of the Royal Society of Chemistry （RSC） and International Fine Particle Research Institute （IFPRI）. The forum was supported financially by the Engineering and Physics Sciences Research Council （EPSRC） of United Kingdom,     

基于鲁棒滤波的捷联导引头视线角速度估计方法

针对捷联导引头无法直接获取视线角速度等信息的问题,研究了鲁棒滤波在大气层外飞行器捷联导引头视线角速度估计中的应用。为了建立非线性滤波估计模型,考虑目标视线角速度的慢变特性,采用一阶马尔科夫模型建立了状态方程;推导了视线角速度的解耦模型,并建立了量测方程;考虑到实际应用中存在系统噪声统计特性失准的问题,基于Huber-Based鲁棒滤波方法,设计了视线角速度滤波器,并完成了基于Huber-Based滤波方法和扩展卡尔曼滤波方法的数学仿真。仿真结果表明Huber-Based滤波方法的视线角、视线角速度及视线角加速度估计精度分别达到0.1140'、0.1423'/s、0.0203'/s2,而扩展卡尔曼滤波方法的视线角、视线角速度及视线角加速度估计精度仅分别为0.6577'、0.6415'/s、0.0979'/s~2。仿真结果证明了该方法可以有效地估计出相对视线角速度等信息,并且在非高斯噪声的条件下,依然可获得较高的估计精度,具有一定的鲁棒性。     

Guide for authors

正Each of the sections below provides essential information for authors.We recommend that you take the time to read them before submitting a contribution to Acta Mechanica Sinica.We hope our guide to authors may help you navigate to the appropriate section.How to prepare a submission This document provides an outline of the editorial process involved in publishing a scientific paper in Acta Mechanica     

Use specification of multiscale materials for life spanned over macro-, micro-, nano-, and pico-scale

Multiscale material intends to enhance the strength and life of mechanical systems by matching the transmitted spatiotemporal energy distribution to the constituents at the different scale, say—macro, micro, nano, and pico,—, depending on the needs. Lower scale entities are, particularly, critical to small size systems. Large structures are less sensitive to microscopic effects. Scale shifting laws will be developed for relating test data from nano-, micro-, and macro-specimens. The benefit of reinforcement at the lower scale constituents needs to be justified at the macroscopic scale. Filling the void and space in regions of high energy density is considered.Material inhomogeneity interacts with specimen size. Their combined effect is non-equilibrium. Energy exchange between the environment and specimen becomes increasingly more significant as the specimen size is reduced. Perturbation of the operational conditions can further aggravate the situation. Scale transitional functions and/or f_j/j+1 are introduced to quantify these characteristics. They are represented, respectively, by , and (f_mi/ma,f_na/mi,f_pi/na). The abbreviations pi, na, mi, and ma refer to pico, nano, micro and macro.Local damage is assumed to initiate at a small scale, grows to a larger scale, and terminate at an even larger scale. The mechanism of energy absorption and dissipation will be introduced to develop a consistent book keeping system. Compaction of mass density for constituents of size 10⁻¹², 10⁻⁹, 10⁻⁶, 10⁻³ m, will be considered. Energy dissipation at all scales must be accounted for. Dissipations at the smaller scale must not only be included but they must abide by the same physical and mathematical interpretation, in order to avoid inconsistencies when making connections with those at the larger scale where dissipations are eminent.Three fundamental Problems I, II, and III are stated. They correspond to the commonly used service conditions. Reference is made to a Representative Tip (RT), the location where energy absorption and dissipation takes place. The RT can be a crack tip or a particle. At the larger size scales, RT can refer to a region. Scale shifting of results from the very small to the very large is needed to identify the benefit of using multiscale materials.